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Fluid Dynamics

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86
MHT CET
34
JEE Main
44
NEET
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Years
2002–2026
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Q1MHT CET 2026 · 20 APR · SHIFT 1Easy

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

In case of liquid, if Reynold's number 'RnR_n' is 14501450, then the flow of liquid will

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Answer: (c)

  1. Reynolds number ranges: Rn<1000R_n < 1000 streamline, 1000<Rn<20001000 < R_n < 2000 unsteady (changing), Rn>2000R_n > 2000 turbulent.
  2. Rn=1450R_n = 1450 lies between 10001000 and 20002000, so the flow is in transition from streamline to turbulent.
  3. So the answer is (c).
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Q2MHT CET 2026 · 18 APR · SHIFT 2Easy

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

In case of fluid flowing on horizontal surface the flow of fluid becomes unsteady when Reynolds number (Rn) is

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Answer: (d)

  1. Reynolds number ranges: Rn<1000R_n < 1000 streamline, 10001000 to 20002000 transition, Rn>2000R_n > 2000 turbulent.
  2. Fully irregular (unsteady, turbulent) flow sets in when Rn>2000R_n > 2000.
  3. So the answer is (d) greater than 2000.
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Q3MHT CET 2026 · 19 APR · SHIFT 1Easy

Types of Flow, Reynolds Number & Continuity · Equation of continuity

An in-compressible fluid flows steadily through a horizontal cylindrical pipe. The pipe has radius '3R3R' at point A and '1.5R1.5R' at point B, further along the flow direction at the same level. If the velocity at point A is 'vv', then that at point B is

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Answer: (d)

  1. Continuity: AAvA=ABvB⇒rA2v=rB2vBA_A v_A = A_B v_B \Rightarrow r_A^2 v = r_B^2 v_B
  2. vB=v(3R1.5R)2=4vv_B = v\left(\dfrac{3R}{1.5R}\right)^2 = 4v
  3. So the answer is (d) 4v4v.
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Q4MHT CET 2026 · 16 APR · SHIFT 1Easy

Types of Flow, Reynolds Number & Continuity · Equation of continuity

Water flows through a horizontal pipe at a speed 'V'. Internal diameter of the pipe is 'd'. If the water is emerging at a speed 'V1V_1 ' then the diameter of the nozzle is

______

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Answer: (a)

  1. Continuity: πd24V=πD24V1\dfrac{\pi d^2}{4}V = \dfrac{\pi D^2}{4}V_1, where DD is the nozzle diameter.
  2. D2=d2VV1⇒D=dVV1D^2 = d^2\dfrac{V}{V_1} \Rightarrow D = d\sqrt{\dfrac{V}{V_1}}
  3. So the answer is (a) dV/V1d\sqrt{V/V_1}.
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Q5JEE Main 2026 · 4 APR · SHIFT 2Easy

Types of Flow, Reynolds Number & Continuity · Equation of continuity

A water spray gun is attached to a hose of cross sectional area 30 cm230\text{ cm}^2. The gun comprises of 10 perforations each of cross sectional area of 15 mm215\text{ mm}^2. If the water flows in the hose with the speed of 50 cm/s50\text{ cm/s}, calculate the speed at which the water flows out from each perforation. (Neglect any edge effects)

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Answer: (b)

  1. Continuity: A1v1=navA_1 v_1 = n a v (all perforations together).
  2. A1v1=30 cm2×50 cm/s=1500 cm3/s=1.5×10−3 m3/sA_1 v_1 = 30\text{ cm}^2 \times 50\text{ cm/s} = 1500\text{ cm}^3/\text{s} = 1.5\times10^{-3}\text{ m}^3/\text{s}
  3. na=10×15 mm2=150 mm2=1.5×10−4 m2na = 10 \times 15\text{ mm}^2 = 150\text{ mm}^2 = 1.5\times10^{-4}\text{ m}^2
  4. v=1.5×10−31.5×10−4=10 m/sv = \dfrac{1.5\times10^{-3}}{1.5\times10^{-4}} = 10\text{ m/s}
  5. So the answer is (b) 10 m/s10\text{ m/s}.
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Q6MHT CET 2025 · 21 APR · SHIFT 2Easy

Types of Flow, Reynolds Number & Continuity · Equation of continuity

Water flows through a horizontal pipe of varying cross-section at the rate of π×10−1 m3/s\pi \times 10^{-1}\text{ m}^3/\text{s}. The velocity of water at a point where the radius of the pipe is 10 cm is (π=3.14)(\pi = 3.14)

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Answer: (c)

  1. Rate of flow Q=Av=πr2vQ = Av = \pi r^2 v.
  2. v=π×10−1π(0.1)2=10−110−2=10 m/sv = \dfrac{\pi \times 10^{-1}}{\pi (0.1)^2} = \dfrac{10^{-1}}{10^{-2}} = 10\text{ m/s}
  3. So the answer is (c) 10 m/s10\text{ m/s}.
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Q7MHT CET 2025 · 21 APR · SHIFT 1Easy

Types of Flow, Reynolds Number & Continuity · Equation of continuity

An incompressible fluid flows steadily through a cylindrical pipe having radius R at point A and (R3)\left(\frac{R}{3}\right) at point B further along the direction of flow of liquid. If the velocity at point A is ' V ' then that at point B is

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Answer: (d)

  1. Continuity: πR2V=π(R/3)2vB\pi R^2 V = \pi (R/3)^2 v_B
  2. vB=9Vv_B = 9V
  3. So the answer is (d) 9V9V.
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Q8MHT CET 2023 · 12 MAY · SHIFT 2Easy

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

Select the WRONG statement from the following. In a streamline flow

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Answer: (a)

  1. In streamline flow, the velocity at a given point stays constant with time, so (a) is wrong.
  2. (b), (c) and (d) are true: speed below critical velocity, parallel layers, no random motion.
  3. So the wrong statement is (a).
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Q9MHT CET 2023 · 11 MAY · SHIFT 2Easy

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

A fluid of density 'ρ\rho' is flowing through a uniform tube of diameter 'dd'. The coefficient of viscosity of the fluid is 'η\eta', then critical velocity of the fluid is

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Answer: (b)

  1. Rn=ρvcdη⇒vc=RnηρdR_n = \dfrac{\rho v_c d}{\eta} \Rightarrow v_c = \dfrac{R_n \eta}{\rho d}
  2. vc∝ηv_c \propto \eta, and vc∝1/ρv_c \propto 1/\rho, vc∝1/dv_c \propto 1/d.
  3. So the answer is (b) directly proportional to η\eta.
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Q10MHT CET 2023 · 9 MAY · SHIFT 2Easy

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

A fluid of density 'ρ\rho' and viscosity 'η\eta' is flowing through a pipe of diameter 'dd', with a velocity 'vv'. Reynold number is

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Answer: (b)

  1. Reynolds number = inertial force / viscous force =ρvdη= \dfrac{\rho v d}{\eta}.
  2. So the answer is (b) dρvη\dfrac{d\rho v}{\eta}.
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Q11MHT CET 2023 · 10 MAY · SHIFT 1Easy

Types of Flow, Reynolds Number & Continuity · Equation of continuity

Water flows through a horizontal pipe at a speed 'VV'. Internal diameter of the pipe is 'dd'. If the water is coming out at a speed 'V1V_1' then the diameter of the nozzle is

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Answer: (b)

  1. Continuity: d2V=D2V1d^2 V = D^2 V_1, where DD is the nozzle diameter.
  2. D=dVV1D = d\sqrt{\dfrac{V}{V_1}}
  3. So the answer is (b).
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Q12JEE Main 2022 · 26 JUN · SHIFT 2Easy

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

If ρ\rho is the density and η\eta is coefficient of viscosity of fluid which flows with a speed v in the pipe of diameter d, the correct formula for Reynolds number Re is:

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Answer: (c)

  1. Reynolds number Re=ρvdηR_e = \dfrac{\rho v d}{\eta} (dimensionless).
  2. So the answer is (c).
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Q13JEE Main 2022 · 28 JUL · SHIFT 2Medium

Types of Flow, Reynolds Number & Continuity · Equation of continuity

A pressure-pump has a horizontal tube of cross sectional area 10 cm210\text{ cm}^2 for the outflow of water at a speed of 20 m/s20\text{ m/s}. The force exerted on the vertical wall just in front of the tube which stops water horizontally flowing out of the tube, is:

[given: density of water =1000 kg/m3= 1000\text{ kg/m}^3]

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Answer: (d)

  1. Force = rate of change of momentum =dmdtv=(ρAv)v=ρAv2= \dfrac{dm}{dt}v = (\rho A v)v = \rho A v^2 (water stopped by the wall).
  2. F=1000×10×10−4×(20)2F = 1000 \times 10\times10^{-4} \times (20)^2
  3. F=400 NF = 400\text{ N}
  4. So the answer is (d) 400 N400\text{ N}.
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Q14JEE Main 2022 · 29 JUN · SHIFT 1Medium

Types of Flow, Reynolds Number & Continuity · Equation of continuity

A block of metal weighing 2 kg is resting on a frictionless plane (as shown in figure). It is struck by a jet releasing water at a rate of 1 kgs−1{}^{-1} and at a speed of 10 ms−1{}^{-1}. Then, the initial acceleration of the block, in ms−2{}^{-2}, will be:

Figure

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Answer: (c)

  1. The jet loses its horizontal momentum on hitting the block: F=dmdtvF = \dfrac{dm}{dt}v.
  2. F=1 kg/s×10 m/s=10 NF = 1\text{ kg/s} \times 10\text{ m/s} = 10\text{ N}
  3. a=Fm=102=5 m/s2a = \dfrac{F}{m} = \dfrac{10}{2} = 5\text{ m/s}^2
  4. So the answer is (c) 5.
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Q15MHT CET 2021 · 24 SEP · SHIFT 1Medium

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

A glass tube of uniform cross-section is connected to a tap with a rubber tube. The tap is opened slowly. Initially the flow of water in the tube is streamline. The speed of flow of water to convert it into a turbulent flow is [radius of tube =1 cm,η=1×10−3 Nsm2,Rn=2500= 1\text{ cm}, \eta = 1 \times 10^{-3}\,\frac{\text{Ns}}{\text{m}^2}, R_n = 2500 and density of water =103 kg/m3= 10^{3}\text{ kg/m}^3 ]

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Answer: (b)

  1. Rn=ρvDη⇒v=RnηρDR_n = \dfrac{\rho v D}{\eta} \Rightarrow v = \dfrac{R_n \eta}{\rho D}, with D=2r=0.02 mD = 2r = 0.02\text{ m}.
  2. v=2500×10−3103×0.02=2.520v = \dfrac{2500 \times 10^{-3}}{10^3 \times 0.02} = \dfrac{2.5}{20}
  3. v=0.125 m/sv = 0.125\text{ m/s}
  4. So the answer is (b) 0.125 m/s0.125\text{ m/s}.
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Q16JEE Main 2021 · 16 MAR · SHIFT 2Medium

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

What will be the nature of flow of water from a circular tap, when its flow rate increased from 0.18 L/min to 0.48 L/min? The radius of the tap and viscosity of water are 0.5 cm and 10−-3 Pa s, respectively. (Density of water: 103 kg/m3)

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Answer: (a)

  1. Re=ρvDηR_e = \dfrac{\rho v D}{\eta} with v=Qπr2v = \dfrac{Q}{\pi r^2} gives Re=2ρQπηrR_e = \dfrac{2\rho Q}{\pi \eta r}.
  2. Q1=0.18 L/min=3×10−6 m3/sQ_1 = 0.18\text{ L/min} = 3\times10^{-6}\text{ m}^3/\text{s}: Re=2×103×3×10−6π×10−3×0.005≈382R_e = \dfrac{2\times10^3\times3\times10^{-6}}{\pi\times10^{-3}\times0.005} \approx 382
  3. Q2=0.48 L/min=8×10−6 m3/sQ_2 = 0.48\text{ L/min} = 8\times10^{-6}\text{ m}^3/\text{s}: Re≈1019R_e \approx 1019
  4. ReR_e goes from below 10001000 (steady) to above 10001000 (unsteady).
  5. So the answer is (a) steady flow to unsteady flow.
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Q17JEE Main 2020 · 7 JAN · SHIFT 2Easy

Types of Flow, Reynolds Number & Continuity · Equation of continuity

An ideal fluid flows (laminar flow) through a pipe of non-uniform diameter. The maximum and minimum diameters of the pipes are 6.4 cm and 4.8 cm, respectively. The ratio of the minimum and the maximum velocities of fluid in this pipe is:

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Answer: (b)

  1. Continuity: v∝1A∝1d2v \propto \dfrac{1}{A} \propto \dfrac{1}{d^2}.
  2. Minimum velocity is at maximum diameter: vminvmax=(dmindmax)2=(4.86.4)2\dfrac{v_{min}}{v_{max}} = \left(\dfrac{d_{min}}{d_{max}}\right)^2 = \left(\dfrac{4.8}{6.4}\right)^2
  3. =(34)2=916= \left(\dfrac{3}{4}\right)^2 = \dfrac{9}{16}
  4. So the answer is (b) 916\dfrac{9}{16}.
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Q18JEE Main 2019 · 8 APR · SHIFT 1Medium

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

Water from a pipe is coming at a rate of 100 litres per minute. If the radius of the pipe is 5 cm, the Reynolds number for the flow is of the order of: (density of water = 1000 kg/m3, coefficient of viscosity of water = 1mPas)

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Answer: (b)

  1. Re=ρvDηR_e = \dfrac{\rho v D}{\eta} with v=Qπr2v = \dfrac{Q}{\pi r^2}, D=2rD = 2r gives Re=2ρQπηrR_e = \dfrac{2\rho Q}{\pi \eta r}.
  2. Q=100 L/min=0.160≈1.67×10−3 m3/sQ = 100\text{ L/min} = \dfrac{0.1}{60} \approx 1.67\times10^{-3}\text{ m}^3/\text{s}
  3. Re=2×1000×1.67×10−3π×10−3×0.05≈2.1×104R_e = \dfrac{2\times1000\times1.67\times10^{-3}}{\pi\times10^{-3}\times0.05} \approx 2.1\times10^{4}
  4. So the answer is (b) of the order of 10410^4.
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Q19JEE Main 2019 · 10 APR · SHIFT 2Medium

Types of Flow, Reynolds Number & Continuity · Equation of continuity

Water from a tap emerges vertically downwards with an initial speed of 1.0 ms–1. The cross- sectional area of the tap is 10–4 m2. Assume that the pressure is constant throughout the stream of water and that the flow is streamlined. The cross-sectional area of the stream, 0.15 m below the tap would be: (Take g = 10 ms–2)

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Answer: (c)

  1. Speed after falling hh: v2=u2+2gh=1+2×10×0.15=4⇒v=2 m/sv^2 = u^2 + 2gh = 1 + 2\times10\times0.15 = 4 \Rightarrow v = 2\text{ m/s}
  2. Continuity: A1u=A2v⇒A2=10−4×12A_1 u = A_2 v \Rightarrow A_2 = \dfrac{10^{-4}\times1}{2}
  3. A2=5×10−5 m2A_2 = 5\times10^{-5}\text{ m}^2
  4. So the answer is (c).
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Q20JEE Main 2019 · 11 JAN · SHIFT 1Medium

Types of Flow, Reynolds Number & Continuity · Equation of continuity

A liquid of density ρ\rho is coming out of a hose pipe of radius a with horizontal speed vv and hits a mesh. 50% of the liquid passes through the mesh unaffected. 25% looses all of its momentum and 25% comes back with the same speed. The resultant pressure on the mesh will be:

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Answer: (a)

  1. Momentum carried per second by the jet =ρAv2= \rho A v^2.
  2. 50% passes through: no momentum change.
  3. 25% stops: change =0.25ρAv2= 0.25\rho A v^2; 25% rebounds with same speed: change =0.25×2ρAv2=0.5ρAv2= 0.25\times 2\rho A v^2 = 0.5\rho A v^2.
  4. F=0.75ρAv2⇒P=FA=34ρv2F = 0.75\rho A v^2 \Rightarrow P = \dfrac{F}{A} = \dfrac{3}{4}\rho v^2
  5. So the answer is (a).
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Q21JEE Main 2015 · 10 APR · SHIFT 1Medium

Types of Flow, Reynolds Number & Continuity · Types of flow & Reynolds number

If it takes 5 minutes to fill a 15 litre bucket from a water tap of diameter 2π\frac{2}{\sqrt{\pi}} cm then the Reynolds number for the flow is (density of water = 103 kg/m3 and viscosity of water = 10−-3 Pa.s) close to:

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Answer: (a)

  1. Q=15×10−35×60=5×10−5 m3/sQ = \dfrac{15\times10^{-3}}{5\times60} = 5\times10^{-5}\text{ m}^3/\text{s}
  2. r=1π cm⇒A=πr2=1 cm2=10−4 m2r = \dfrac{1}{\sqrt{\pi}}\text{ cm} \Rightarrow A = \pi r^2 = 1\text{ cm}^2 = 10^{-4}\text{ m}^2, so v=QA=0.5 m/sv = \dfrac{Q}{A} = 0.5\text{ m/s}
  3. Re=ρvDη=103×0.5×2π×10−210−3≈5.6×103R_e = \dfrac{\rho v D}{\eta} = \dfrac{10^3 \times 0.5 \times \frac{2}{\sqrt{\pi}}\times10^{-2}}{10^{-3}} \approx 5.6\times10^{3}
  4. So the answer is (a) about 55005500.
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Q22JEE Main 2011 · AIEEEMedium

Types of Flow, Reynolds Number & Continuity · Equation of continuity

Water is flowing continuously from a tap having an internal diameter 8×10−3 m.8 \times 10^{-3}\text{ m.} The water velocity as it leaves the tap is 0.4 ms−10.4\text{ ms}^{-1}. The diameter of the water stream at a distance 2×10−1 m2 \times 10^{-1}\text{ m} below the tap is close to:

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Answer: (c)

  1. Speed at h=0.2 mh = 0.2\text{ m} below: v2=(0.4)2+2×10×0.2=4.16⇒v≈2.04 m/sv^2 = (0.4)^2 + 2\times10\times0.2 = 4.16 \Rightarrow v \approx 2.04\text{ m/s}
  2. Continuity: d12v1=d22v2⇒d2=d1v1v2d_1^2 v_1 = d_2^2 v_2 \Rightarrow d_2 = d_1\sqrt{\dfrac{v_1}{v_2}}
  3. d2=8×10−30.42.04≈8×10−3×0.44≈3.6×10−3 md_2 = 8\times10^{-3}\sqrt{\dfrac{0.4}{2.04}} \approx 8\times10^{-3}\times0.44 \approx 3.6\times10^{-3}\text{ m}
  4. So the answer is (c).
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Q23MHT CET 2026 · 18 APR · SHIFT 2Medium

Bernoulli's Equation

An incompressible fluid (ideal fluid) is flowing through non uniform cross-sectional tube PQ as shown in the figure from end P to end Q. If KPK_P and KQK_Q are the kinetic energy per unit volume of the fluid at end P and end Q respectively, then

Figure

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Answer: (d)

  1. From the figure AP<AQA_P < A_Q; continuity APvP=AQvQA_P v_P = A_Q v_Q gives vP>vQv_P > v_Q.
  2. KE per unit volume K=12ρv2K = \frac{1}{2}\rho v^2, so KP>KQK_P > K_Q.
  3. So the answer is (d).
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Q24MHT CET 2026 · 16 APR · SHIFT 2Medium

Bernoulli's Equation

A horizontal pipe carries water in a streamline flow. At point along the pipe, where the cross- sectional area is A1A_1, the velocity of water is V1V_1 and the pressure is P1P_1. What is the pressure of water at another point where the cross-sectional area is A2A_2?

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Answer: (b)

  1. Continuity: V2=A1V1A2V_2 = \dfrac{A_1 V_1}{A_2}
  2. Bernoulli (horizontal): P2=P1+12ρ(V12−V22)=P1+12ρV12(1−A12A22)P_2 = P_1 + \frac{1}{2}\rho (V_1^2 - V_2^2) = P_1 + \frac{1}{2}\rho V_1^2\left(1 - \dfrac{A_1^2}{A_2^2}\right)
  3. P2=P1+ρV122A22(A22−A12)P_2 = P_1 + \dfrac{\rho V_1^2}{2A_2^2}(A_2^2 - A_1^2)
  4. So the answer is (b).
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Q25MHT CET 2026 · 16 APR · SHIFT 1Medium

Bernoulli's Equation

A closed pipe containing liquid showed a pressure P1P_1 by gauge. When the valve was opened, pressure was reduced to P2P_2. The speed of water flowing out of the pipe is (ρ\rho=density of water)

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Answer: (b)

  1. Closed valve: v=0v = 0, pressure P1P_1. Open valve: pressure P2P_2, speed vv.
  2. Bernoulli: P1=P2+12ρv2P_1 = P_2 + \frac{1}{2}\rho v^2
  3. v=[2(P1−P2)ρ]1/2v = \left[\dfrac{2(P_1 - P_2)}{\rho}\right]^{1/2}
  4. So the answer is (b).
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Q26NEET 2026 · RE-NEETMedium

Bernoulli's Equation

Water flows in a streamline motion through a horizontal pipe of circular cross-section as shown in the figure. The pressure difference of water between PP and QQ is 15 Nm−215\text{ Nm}^{-2}. The area of cross-section at PP and QQ are 40 cm240\text{ cm}^2 and 20 cm220\text{ cm}^2, respectively. The rate of flow of water through the pipe, in cm3 s−1\text{cm}^3\text{ s}^{-1}, is:

[Take density of water =1000 kg m−3= 1000\text{ kg m}^{-3} ]

Figure

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Answer: (a)

  1. Continuity: vQ=4020vP=2vPv_Q = \dfrac{40}{20}v_P = 2v_P
  2. Bernoulli: PP−PQ=12ρ(vQ2−vP2)=32ρvP2P_P - P_Q = \frac{1}{2}\rho(v_Q^2 - v_P^2) = \frac{3}{2}\rho v_P^2
  3. 15=1500 vP2⇒vP=0.1 m/s=10 cm/s15 = 1500\,v_P^2 \Rightarrow v_P = 0.1\text{ m/s} = 10\text{ cm/s}
  4. Q=APvP=40×10=400 cm3/sQ = A_P v_P = 40\times10 = 400\text{ cm}^3/\text{s}
  5. So the answer is (a) 400.
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Q27JEE Main 2026 · 8 APR · SHIFT 2Medium

Bernoulli's Equation

A liquid of density 600 kg/m3600\text{ kg/m}^3 flowing steadily in a tube of varying cross-section. The cross-section at a point AA is 1.0 cm21.0\text{ cm}^2 and that at BB is 20 mm220\text{ mm}^2. Both the points AA and BB are in same horizontal plane, the speed of the liquid at AA is 10 cm/s10\text{ cm/s}. The difference in pressures at AA and BB points is ______ Pa.

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Answer: (d)

  1. AA=1.0 cm2=100 mm2A_A = 1.0\text{ cm}^2 = 100\text{ mm}^2, AB=20 mm2A_B = 20\text{ mm}^2, so vB=5vA=50 cm/s=0.5 m/sv_B = 5v_A = 50\text{ cm/s} = 0.5\text{ m/s}
  2. Bernoulli: PA−PB=12ρ(vB2−vA2)=12×600×(0.25−0.01)P_A - P_B = \frac{1}{2}\rho(v_B^2 - v_A^2) = \frac{1}{2}\times600\times(0.25 - 0.01)
  3. PA−PB=300×0.24=72 PaP_A - P_B = 300 \times 0.24 = 72\text{ Pa}
  4. So the answer is (d) 72.
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Q28JEE Main 2026 · 21 JAN · SHIFT 1Medium

Bernoulli's Equation

Water flows through a horizontal tube as shown in the figure. The difference in height between the water columns in vertical tubes is 5 cm and the area of cross-sections at AA and BB are 6 cm26\text{ cm}^2 and 3 cm23\text{ cm}^2 respectively. The rate of flow will be ‾ cm3/s\underline{\hspace{3em}}\ \text{cm}^3/\text{s}. (take g=10 m/s2g = 10\text{ m/s}^2)

Figure

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Answer: (d)

  1. Pressure difference from the columns: PA−PB=ρghP_A - P_B = \rho g h.
  2. Bernoulli: 12(vB2−vA2)=gh=10×0.05=0.5⇒vB2−vA2=1\frac{1}{2}(v_B^2 - v_A^2) = gh = 10\times0.05 = 0.5 \Rightarrow v_B^2 - v_A^2 = 1
  3. Continuity: vB=63vA=2vA⇒3vA2=1⇒vA=13 m/s=1003 cm/sv_B = \dfrac{6}{3}v_A = 2v_A \Rightarrow 3v_A^2 = 1 \Rightarrow v_A = \dfrac{1}{\sqrt{3}}\text{ m/s} = \dfrac{100}{\sqrt{3}}\text{ cm/s}
  4. Q=AAvA=6×1003=2003 cm3/sQ = A_A v_A = 6\times\dfrac{100}{\sqrt{3}} = 200\sqrt{3}\text{ cm}^3/\text{s}
  5. So the answer is (d).
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Q29MHT CET 2025 · 25 APR · SHIFT 2Medium

Bernoulli's Equation

A horizontal pipeline carries water in a streamline flow. At a point along the pipe, where the cross- sectional area is 10 cm210\text{ cm}^2, the velocity of water is 1 m/s1\text{ m/s} and pressure is 2000 Pa. The pressure of water at another point where the cross-sectional area 5 cm25\text{ cm}^2 is

[Given →\rightarrow density of water =1000 kg/m3= 1000\text{ kg/m}^3 ]

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Answer: (c)

  1. Continuity: v2=105×1=2 m/sv_2 = \dfrac{10}{5}\times 1 = 2\text{ m/s}
  2. Bernoulli: P2=P1−12ρ(v22−v12)=2000−12×1000×(4−1)P_2 = P_1 - \frac{1}{2}\rho (v_2^2 - v_1^2) = 2000 - \frac{1}{2}\times1000\times(4 - 1)
  3. P2=2000−1500=500 PaP_2 = 2000 - 1500 = 500\text{ Pa}
  4. So the answer is (c) 500 Pa.
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Q30JEE Main 2025 · 23 JAN · SHIFT 2Medium

Bernoulli's Equation

Water flows in a horizontal pipe whose one end is closed with a valve. The reading of the pressure gauge attached to the pipe is P1P_1. The reading of the pressure gauge falls to P2P_2 when the valve is opened. The speed of water flowing in the pipe is proportional to

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Answer: (b)

  1. Closed valve: v=0v = 0, gauge reads P1P_1. Open valve: gauge reads P2P_2 with speed vv.
  2. Bernoulli: P1−P2=12ρv2⇒v=2(P1−P2)ρP_1 - P_2 = \frac{1}{2}\rho v^2 \Rightarrow v = \sqrt{\dfrac{2(P_1 - P_2)}{\rho}}
  3. So v∝P1−P2v \propto \sqrt{P_1 - P_2}, answer (b).
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Q31JEE Main 2025 · 22 JAN · SHIFT 2Difficult

Bernoulli's Equation

Figure

A tube of length LL is shown in the figure. The radius of cross section at the point (1)(1) is 2 cm and at the point (2) is 1 cm, respectively. If the velocity of water entering at point (1) is 2 m/s2\text{ m/s}, then velocity of water leaving the point (2) will be

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Answer: (d)

  1. Continuity: πr12v1=πr22v2⇒v2=(r1r2)2v1\pi r_1^2 v_1 = \pi r_2^2 v_2 \Rightarrow v_2 = \left(\frac{r_1}{r_2}\right)^2 v_1
  2. v2=(21)2(2)=8 m/sv_2 = \left(\frac{2}{1}\right)^2 (2) = 8\text{ m/s}
  3. So the answer is (d) 8 m/s.
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Q32JEE Main 2024 · 8 APR · SHIFT 1Easy

Bernoulli's Equation

Correct Bernoulli's equation is (symbols have their usual meaning):

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Answer: (d)

  1. Bernoulli: pressure energy + potential energy + kinetic energy per unit volume is constant.
  2. P+ρgh+12ρv2=P + \rho g h + \frac{1}{2}\rho v^2 = constant
  3. So the answer is (d).
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Q33MHT CET 2024 · 10 MAY · SHIFT 1Medium

Bernoulli's Equation

A closed pipe containing a liquid showed a pressure P1P_1 by gauge. When the valve was opened, pressure was reduced to P2P_2. The speed of water flowing out of the pipe is (ρ=\rho = density of water)

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Answer: (c)

  1. Closed valve: v=0v = 0, pressure P1P_1. Open valve: pressure P2P_2, speed vv.
  2. Bernoulli: P1−P2=12ρv2P_1 - P_2 = \frac{1}{2}\rho v^2
  3. v=[2(P1−P2)ρ]1/2v = \left[\dfrac{2(P_1 - P_2)}{\rho}\right]^{1/2}
  4. So the answer is (c).
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Q34MHT CET 2024 · 9 MAY · SHIFT 1Medium

Bernoulli's Equation

Water is flowing in a conical tube as shown in figure. Velocity of water at area ' A2A_2 ' is 60 cm/s60\text{ cm/s}. The value of ' A1A_1 ' and ' A2A_2 ' is 10 cm210\text{ cm}^2 and 5 cm25\text{ cm}^2 respectively. The pressure difference at both the cross- section is

Figure

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Answer: (c)

  1. Continuity: v1=A2v2A1=5×0.610=0.3 m/sv_1 = \dfrac{A_2 v_2}{A_1} = \dfrac{5\times0.6}{10} = 0.3\text{ m/s}
  2. Bernoulli (horizontal): P1−P2=12ρ(v22−v12)=12×1000×(0.36−0.09)P_1 - P_2 = \frac{1}{2}\rho (v_2^2 - v_1^2) = \frac{1}{2}\times1000\times(0.36 - 0.09)
  3. P1−P2=500×0.27=135 N/m2P_1 - P_2 = 500 \times 0.27 = 135\text{ N/m}^2
  4. So the answer is (c).
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Q35MHT CET 2024 · 2 MAY · SHIFT 1Medium

Bernoulli's Equation

A streamline flow of a liquid of density ' ρ\rho ' is passing through a horizontal pipe of crosssectional area A1A_1 and A2A_2 at two ends. If the pressure of liquid is ' P ' at a point where flow speed is ' vv ', then pressure at another point where the flow of speed becomes 3 v is

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Answer: (d)

  1. Bernoulli (horizontal): P+12ρv2=P′+12ρ(3v)2P + \frac{1}{2}\rho v^2 = P' + \frac{1}{2}\rho (3v)^2
  2. P′=P−12ρ(9v2−v2)=P−4ρv2P' = P - \frac{1}{2}\rho(9v^2 - v^2) = P - 4\rho v^2
  3. So the answer is (d).
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Q36NEET 2024Medium

Bernoulli's Equation

An ideal fluid is flowing in a non-uniform cross-sectional tube XYXY (as shown in the figure) from end XX to end YY. If K1K_1 and K2K_2 are the kinetic energy per unit volume of the fluid at XX and YY respectively, then the correct option is:

Figure

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Answer: (c)

  1. From the figure, end XX is narrow and end YY is wide: AX<AYA_X < A_Y.
  2. Continuity AXvX=AYvYA_X v_X = A_Y v_Y gives vX>vYv_X > v_Y.
  3. KE per unit volume =12ρv2= \frac{1}{2}\rho v^2, so K1>K2K_1 > K_2 (height does not affect it).
  4. So the answer is (c).
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Q37MHT CET 2024 · 2 MAY · SHIFT 1Difficult

Bernoulli's Equation

Glycerine of density 1.25×103 kg/m31.25 \times 10^{3}\text{ kg/m}^3 is flowing in conical shaped horizontal pipe. Crosssectional area of the pipe at its both ends is 10 cm210\text{ cm}^2 and 5 cm25\text{ cm}^2 respectively. Pressure difference at both the ends is 3 N/m23\text{ N/m}^2. Rate of flow of liquid in the pipe is

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Answer: (a)

  1. Continuity: v2=105v1=2v1v_2 = \frac{10}{5}v_1 = 2v_1
  2. Bernoulli: ΔP=12ρ(4v12−v12)⇒3=12(1250)(3v12)\Delta P = \frac{1}{2}\rho(4v_1^2 - v_1^2) \Rightarrow 3 = \frac{1}{2}(1250)(3v_1^2)
  3. v12=1.6×10−3⇒v1=0.04 m/sv_1^2 = 1.6\times10^{-3} \Rightarrow v_1 = 0.04\text{ m/s}
  4. Q=A1v1=(10×10−4)(0.04)=4×10−5 m3/sQ = A_1v_1 = (10\times10^{-4})(0.04) = 4\times10^{-5}\text{ m}^3\text{/s}
  5. So the answer is (a) 4×10−5 m3/s4\times10^{-5}\text{ m}^3\text{/s}.
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Q38MHT CET 2023 · 9 MAY · SHIFT 1Easy

Bernoulli's Equation

Water is flowing through a horizontal pipe in stream line flow. At the narrowest part of the pipe

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Answer: (a)

  1. Continuity: AvAv = constant, so the speed is largest where AA is smallest.
  2. Bernoulli (horizontal): P+12ρv2P + \frac{1}{2}\rho v^2 = constant, so larger vv means smaller PP.
  3. So the answer is (a) velocity maximum, pressure minimum.
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Q39JEE Main 2023 · 13 APR · SHIFT 1Medium

Bernoulli's Equation

Figure

The figure shows a liquid of given density flowing steadily in horizontal tube of varying cross - section. Cross sectional areas at AA is 1.5 cm21.5\text{ cm}^2, and BB is 25 mm225\text{ mm}^2, if the speed of liquid at BB is 60 cm/s60\text{ cm/s} then (PA−PB)(P_A - P_B) is:

(Given PAP_A and PBP_B are liquid pressures at AA and BB points.

density ρ=1000 kg m−3\rho = 1000\text{ kg m}^{-3}

AA and BB are on the axis of tube

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Answer: (b)

  1. AA=1.5 cm2=150 mm2A_A = 1.5\text{ cm}^2 = 150\text{ mm}^2, AB=25 mm2A_B = 25\text{ mm}^2.
  2. Continuity: vA=25150×0.6=0.1 m/sv_A = \dfrac{25}{150}\times 0.6 = 0.1\text{ m/s}
  3. Bernoulli: PA−PB=12×1000×(0.36−0.01)=500×0.35P_A - P_B = \frac{1}{2}\times1000\times(0.36 - 0.01) = 500\times0.35
  4. PA−PB=175 PaP_A - P_B = 175\text{ Pa}
  5. So the answer is (b).
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Q40JEE Main 2023 · 12 APR · SHIFT 1Medium

Bernoulli's Equation

Glycerin of density 1.25×103 kg m−31.25 \times 10^{3}\text{ kg m}^{-3} is flowing through the conical section of pipe. The area of cross-section of the pipe at its ends are 10 cm210\text{ cm}^2 and 5 cm25\text{ cm}^2 and pressure drop across its length is 3 Nm−23\text{ Nm}^{-2}. The rate of flow of glycerin through the pipe is x×10−5 m3 s−1x \times 10^{-5}\text{ m}^3\text{ s}^{-1}. The value of xx is ___________.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 4

  1. Continuity: A1v1=A2v2⇒v2=105v1=2v1A_1v_1 = A_2v_2 \Rightarrow v_2 = \frac{10}{5}v_1 = 2v_1
  2. Bernoulli (horizontal): ΔP=12ρ(v22−v12)=12ρ(3v12)\Delta P = \frac{1}{2}\rho(v_2^2 - v_1^2) = \frac{1}{2}\rho(3v_1^2)
  3. 3=12(1250)(3v12)⇒v12=1.6×10−3⇒v1=0.04 m/s3 = \frac{1}{2}(1250)(3v_1^2) \Rightarrow v_1^2 = 1.6\times10^{-3} \Rightarrow v_1 = 0.04\text{ m/s}
  4. Q=A1v1=(10×10−4)(0.04)=4×10−5 m3/sQ = A_1v_1 = (10\times10^{-4})(0.04) = 4\times10^{-5}\text{ m}^3\text{/s}
  5. So x=4x = 4.
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Q41JEE Main 2023 · 10 APR · SHIFT 2Difficult

Bernoulli's Equation

Figure below shows a liquid being pushed out of the tube by a piston having area of cross section 2.0 cm22.0\text{ cm}^2. The area of cross section at the outlet is 10 mm210\text{ mm}^2. If the piston is pushed at a speed of 4 cm s−14\text{ cm s}^{-1}, the speed of outgoing fluid is __________ cms−1\text{cms}^{-1}

Figure

Numerical answer type. Work it out, then open the answer.

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Answer: 80

  1. Continuity: A1v1=A2v2A_1v_1 = A_2v_2, with A1=2.0 cm2=200 mm2A_1 = 2.0\text{ cm}^2 = 200\text{ mm}^2
  2. v2=20010×4=80 cm/sv_2 = \frac{200}{10}\times 4 = 80\text{ cm/s}
  3. So the answer is 8080 cm s−1^{-1}.
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Q42JEE Main 2022 · 28 JUN · SHIFT 2Medium

Bernoulli's Equation

A liquid of density 750 kgm−3{}^{-3} flows smoothly through a horizontal pipe that tapers in cross- sectional area from A1 = 1.2 ×\times 10−-2 m2 to A2 = A12\frac{A_1}{2}. The pressure difference between the wide and narrow sections of the pipe is 4500 Pa. The rate of flow of liquid is ___________ ×\times 10−-3 m3s−1{}^{-1}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 24

  1. Continuity: A2=A12⇒v2=2v1A_2 = \frac{A_1}{2} \Rightarrow v_2 = 2v_1
  2. Bernoulli: ΔP=12ρ(v22−v12)=32ρv12\Delta P = \frac{1}{2}\rho(v_2^2 - v_1^2) = \frac{3}{2}\rho v_1^2
  3. 4500=32(750)v12=1125 v12⇒v1=2 m/s4500 = \frac{3}{2}(750)v_1^2 = 1125\,v_1^2 \Rightarrow v_1 = 2\text{ m/s}
  4. Q=A1v1=(1.2×10−2)(2)=24×10−3 m3/sQ = A_1v_1 = (1.2\times10^{-2})(2) = 24\times10^{-3}\text{ m}^3\text{/s}
  5. So the answer is 2424.
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Q43JEE Main 2022 · 26 JUN · SHIFT 1Medium

Bernoulli's Equation

An ideal fluid of density 800 kgm−3{}^{-3}, flows smoothly through a bent pipe (as shown in figure) that tapers in cross-sectional area from a to a2\frac{a}{2}. The pressure difference between the wide and narrow sections of pipe is 4100 Pa. At wider section, the velocity of fluid is x6\frac{\sqrt{x}}{6} ms−1{}^{-1} for x = ___________. (Given g = 10 ms−2{}^{-2})

Figure

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 363

  1. Continuity: area a→a2a \to \frac{a}{2}, so v2=2v1v_2 = 2v_1. The wide end is h=1h = 1 m higher.
  2. Bernoulli: P1+12ρv12+ρgh=P2+12ρv22P_1 + \frac{1}{2}\rho v_1^2 + \rho g h = P_2 + \frac{1}{2}\rho v_2^2
  3. (P1−P2)+ρgh=32ρv12⇒4100+800(10)(1)=32(800)v12(P_1 - P_2) + \rho g h = \frac{3}{2}\rho v_1^2 \Rightarrow 4100 + 800(10)(1) = \frac{3}{2}(800)v_1^2
  4. 12100=1200 v12⇒v1=1112=1136=3636 m/s12100 = 1200\,v_1^2 \Rightarrow v_1 = \frac{11}{\sqrt{12}} = \frac{11\sqrt{3}}{6} = \frac{\sqrt{363}}{6}\text{ m/s}
  5. So x=363x = 363.
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Q44JEE Main 2022 · 29 JUL · SHIFT 2Difficult

Bernoulli's Equation

A tube of length 50 cm50\text{ cm} is filled completely with an incompressible liquid of mass 250 g250\text{ g} and closed at both ends. The tube is then rotated in horizontal plane about one of its ends with a uniform angular velocity xF rad s−1x\sqrt{F}\text{ rad s}^{-1}. If FF be the force exerted by the liquid at the other end then the value of xx will be __________.

Numerical answer type. Work it out, then open the answer.

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Answer: 4

  1. The liquid moves in a circle; the end wall supplies the total centripetal force, acting on the centre of mass at L2\frac{L}{2}.
  2. F=mω2L2=(0.25)ω2(0.25)=ω216F = m\omega^2\frac{L}{2} = (0.25)\omega^2(0.25) = \frac{\omega^2}{16}
  3. ω=4F rad/s\omega = 4\sqrt{F}\text{ rad/s}
  4. So x=4x = 4.
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Q45JEE Main 2020 · 6 SEP · SHIFT 2Medium

Bernoulli's Equation

A fluid is flowing through a horizontal pipe of varying cross-section, with

speed v ms–1 at a point where the pressure is P pascal. At another point where pressure is P2\frac{P}{2} Pascal its speed is V ms–1. If the density of the fluid is ρ\rho kg m–3 and the flow is streamline, then V is equal to:

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Answer: (b)

  1. Bernoulli (horizontal): P+12ρv2=P2+12ρV2P + \frac{1}{2}\rho v^2 = \dfrac{P}{2} + \frac{1}{2}\rho V^2
  2. P2=12ρ(V2−v2)⇒V2=Pρ+v2\dfrac{P}{2} = \frac{1}{2}\rho(V^2 - v^2) \Rightarrow V^2 = \dfrac{P}{\rho} + v^2
  3. So the answer is (b) Pρ+v2\sqrt{\dfrac{P}{\rho} + v^2}.
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Q46JEE Main 2020 · 9 JAN · SHIFT 1Medium

Bernoulli's Equation

Water flows in a horizontal tube (see figure).

The pressure of water changes by 700 Nm–2

between A and B where the area of cross section

are 40 cm2 and 20 cm2, respectively. Find the

rate of flow of water through the tube.

(density of water = 1000 kgm–3)

Figure

Show answer and solution

Answer: (d)

  1. Continuity: vB=4020vA=2vAv_B = \dfrac{40}{20}v_A = 2v_A
  2. Bernoulli: PA−PB=12ρ(4vA2−vA2)=1500 vA2=700P_A - P_B = \frac{1}{2}\rho(4v_A^2 - v_A^2) = 1500\,v_A^2 = 700
  3. vA2=0.467⇒vA≈0.683 m/s=68.3 cm/sv_A^2 = 0.467 \Rightarrow v_A \approx 0.683\text{ m/s} = 68.3\text{ cm/s}
  4. Q=AAvA=40×68.3≈2732 cm3/sQ = A_A v_A = 40\times68.3 \approx 2732\text{ cm}^3/\text{s}
  5. So the answer is (d) 2720 cm3/s2720\text{ cm}^3/\text{s}.
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Q47NEET 2013Medium

Bernoulli's Equation

A fluid is in streamline flow across a horizontal pipe of variable area of cross section. For this which of the following statements is correct?

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Answer: (a)

  1. Continuity: speed is maximum where the area is minimum (narrowest part).
  2. Bernoulli (horizontal): pressure is maximum where speed is minimum (widest part).
  3. So the answer is (a).
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Q48MHT CET 2025 · 23 APR · SHIFT 1Medium

Applications of Bernoulli's Theorem

A wind with speed 50 m/s50\text{ m/s} blows parallel to the roof of a house. The area of the roof is 300 m2300\text{ m}^2. Assume that the pressure inside the house is atmospheric pressure. Density of air is 1.2 kg/m31.2\text{ kg/m}^3. The magnitude of the force exerted by the wind on the roof will be

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Answer: (c)

  1. Air inside is at rest, air above moves at vv: ΔP=12ρv2\Delta P = \frac{1}{2}\rho v^2
  2. ΔP=12(1.2)(50)2=1500 Pa\Delta P = \frac{1}{2}(1.2)(50)^2 = 1500\text{ Pa}
  3. F=ΔP⋅A=1500×300=4.5×105 NF = \Delta P \cdot A = 1500 \times 300 = 4.5\times10^{5}\text{ N}
  4. So the answer is (c) 4.5×1054.5\times10^{5} N.
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Q49JEE Main 2024 · 1 FEB · SHIFT 1Medium

Applications of Bernoulli's Theorem

A plane is in level flight at constant speed and each of its two wings has an area of 40 m240\text{ m}^2. If the speed of the air is 180 km/h180\text{ km/h} over the lower wing surface and 252 km/h252\text{ km/h} over the upper wing surface, the mass of the plane is ___________ kg.

(Take air density to be 1 kg m−31\text{ kg m}^{-3} and g=10 ms−2g = 10\text{ ms}^{-2})

Numerical answer type. Work it out, then open the answer.

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Answer: 9600

  1. 180 km/h=50 m/s180\text{ km/h} = 50\text{ m/s}, 252 km/h=70 m/s252\text{ km/h} = 70\text{ m/s}
  2. ΔP=12ρ(vu2−vl2)=12(1)(4900−2500)=1200 Pa\Delta P = \frac{1}{2}\rho(v_u^2 - v_l^2) = \frac{1}{2}(1)(4900 - 2500) = 1200\text{ Pa}
  3. Lift on both wings: F=ΔP×2A=1200×80=96000 NF = \Delta P \times 2A = 1200 \times 80 = 96000\text{ N}
  4. mg=F⇒m=9600010=9600 kgmg = F \Rightarrow m = \frac{96000}{10} = 9600\text{ kg}
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Q50JEE Main 2024 · 29 JAN · SHIFT 1Medium

Applications of Bernoulli's Theorem

In a test experiment on a model aeroplane in wind tunnel, the flow speeds on the upper and lower surfaces of the wings are 70 ms−170\text{ ms}^{-1} and 65 ms−165\text{ ms}^{-1} respectively. If the wing area is 2 m22\text{ m}^2, the lift of the wing is _________ NN.

(Given density of air =1.2 kg m−3= 1.2\text{ kg m}^{-3})

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 810

  1. ΔP=12ρ(vu2−vl2)=12(1.2)(702−652)=0.6×675=405 Pa\Delta P = \frac{1}{2}\rho(v_u^2 - v_l^2) = \frac{1}{2}(1.2)(70^2 - 65^2) = 0.6 \times 675 = 405\text{ Pa}
  2. Lift =ΔP×A=405×2=810 N= \Delta P \times A = 405 \times 2 = 810\text{ N}
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Q51MHT CET 2023 · 13 MAY · SHIFT 1Easy

Applications of Bernoulli's Theorem

Venturimeter is used to

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Answer: (c)

  1. A venturimeter measures the pressure difference between the wide and narrow (throat) sections.
  2. Using Bernoulli's equation and continuity, this pressure difference gives the flow speed and hence the volume flow rate.
  3. So the answer is (c) measure rate of flow of liquids.
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Q52NEET 2023Easy

Applications of Bernoulli's Theorem

The venturi-meter works on:

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Answer: (a)

  1. A venturimeter relates the pressure drop at the throat to the flow speed using P+12ρv2=constantP + \frac{1}{2}\rho v^2 = \text{constant}.
  2. So the answer is (a) Bernoulli's principle.
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Q53JEE Main 2023 · 29 JAN · SHIFT 2Medium

Applications of Bernoulli's Theorem

A fully loaded boeing aircraft has a mass of 5.4×1055.4 \times 10^{5} kg. Its total wing area is 500 m2^{2}. It is in level flight with a speed of 1080 km/h. If the density of air ρ\rho is 1.2 kg m−3^{-3}, the fractional increase in the speed of the air on the upper surface of the wing relative to the lower surface in percentage will be. (g=10 m/s2g = 10\text{ m/s}^2)

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Answer: (d)

  1. Level flight: lift =mg⇒ΔP=mgA=5.4×106500=1.08×104 Pa= mg \Rightarrow \Delta P = \frac{mg}{A} = \frac{5.4\times10^{6}}{500} = 1.08\times10^{4}\text{ Pa}
  2. Bernoulli: ΔP=12ρ(vu2−vl2)≈ρv Δv\Delta P = \frac{1}{2}\rho(v_u^2 - v_l^2) \approx \rho v\,\Delta v, with v=1080 km/h=300 m/sv = 1080\text{ km/h} = 300\text{ m/s}
  3. Δv=1.08×1041.2×300=30 m/s\Delta v = \frac{1.08\times10^{4}}{1.2 \times 300} = 30\text{ m/s}
  4. Δvv=30300=0.1=10%\frac{\Delta v}{v} = \frac{30}{300} = 0.1 = 10\%
  5. So the answer is (d) 10.
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Q54MHT CET 2019 · 2 MAY · SHIFT 2Easy

Applications of Bernoulli's Theorem

Two light balls are suspended as shown in figure. When a stream of air passes through the space between them, the distance between the balls will

Figure

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Answer: (d)

  1. Air blown between the balls moves fast there, so by Bernoulli's principle the pressure between them drops.
  2. The still air outside is at higher pressure and pushes the balls inward.
  3. So the answer is (d) decrease.
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Q55NEET 2015 · AIPMT · CANCELLED PAPERMedium

Applications of Bernoulli's Theorem

A wind with speed 40 m/s blows parallel to the roof of a house. The area of the roof is 250 m2. Assuming that the pressure inside the house is atmospheric pressure, the force exerted by the wind on the roof and the direction of the force will be (ρair=1.2 kg/m3)(\rho_{air} = 1.2\, kg/m^3)

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Answer: (a)

  1. Pressure above the roof is lower: ΔP=12ρv2=12(1.2)(40)2=960 Pa\Delta P = \frac{1}{2}\rho v^2 = \frac{1}{2}(1.2)(40)^2 = 960\text{ Pa}
  2. F=ΔP⋅A=960×250=2.4×105 NF = \Delta P \cdot A = 960 \times 250 = 2.4\times10^{5}\text{ N}
  3. Higher pressure is inside, so the force acts upwards.
  4. So the answer is (a) 2.4×1052.4\times10^{5} N, upwards.
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Q56JEE Main 2014 · 19 APR · SHIFT 1Medium

Applications of Bernoulli's Theorem

Figure

In the diagram shown, if the difference in the two tubes of the manometer is 5 cm, the cross section of the tube at A and B is 6 mm2 and 10 mm2 respectively. The rate at which water flows through the tube ( g = 10 ms−2{}^{-2})

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Answer: (a)

  1. Manometer: ΔP=ρgh=1000(10)(0.05)=500 Pa\Delta P = \rho g h = 1000(10)(0.05) = 500\text{ Pa}
  2. Bernoulli: 12ρ(vA2−vB2)=ρgh⇒vA2−vB2=2gh=1\frac{1}{2}\rho(v_A^2 - v_B^2) = \rho g h \Rightarrow v_A^2 - v_B^2 = 2gh = 1
  3. Continuity: 6vA=10vB⇒vB=0.6vA6v_A = 10v_B \Rightarrow v_B = 0.6v_A, so 0.64vA2=1⇒vA=1.25 m/s0.64v_A^2 = 1 \Rightarrow v_A = 1.25\text{ m/s}
  4. Q=AAvA=(6×10−6)(1.25)=7.5×10−6 m3/s=7.5 cc/sQ = A_Av_A = (6\times10^{-6})(1.25) = 7.5\times10^{-6}\text{ m}^3\text{/s} = 7.5\text{ cc/s}
  5. So the answer is (a) 7.5 cc/s.
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Q57JEE Main 2013 · 22 APR · SHIFT 1Medium

Applications of Bernoulli's Theorem

Air of density 1.2 kg m−3^{-3} is blowing across the horizontal wings of an aeroplane in such a way that its speeds above and below the wings are 150 ms−1^{-1} and 100 ms −1^{-1}, respectively. The pressure difference between the upper and lower sides of the wings, is:

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Answer: (c)

  1. Bernoulli: ΔP=12ρ(v12−v22)\Delta P = \frac{1}{2}\rho(v_1^2 - v_2^2)
  2. ΔP=12(1.2)(1502−1002)=0.6×12500=7500 N m−2\Delta P = \frac{1}{2}(1.2)(150^2 - 100^2) = 0.6 \times 12500 = 7500\text{ N m}^{-2}
  3. So the answer is (c) 7500 N m−2^{-2}.
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Q58MHT CET 2026 · 12 MAY · SHIFT 2Medium

Velocity of Efflux (Torricelli)

A water tank of height ’h’\text{'}h\text{'} has a hole at the bottom. It is completely filled with water. The total pressure at the bottom is 4H4H and atmospheric pressure is HH. The velocity of water flowing out of the hole is (ρ\rho = density of water)

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Answer: (a)

  1. Gauge pressure at the bottom: ρgh=4H−H=3H\rho g h = 4H - H = 3H
  2. Torricelli: 12ρv2=ρgh=3H\frac{1}{2}\rho v^2 = \rho g h = 3H
  3. v=6Hρv = \sqrt{\frac{6H}{\rho}}
  4. So the answer is (a) (6Hρ)1/2\left(\frac{6H}{\rho}\right)^{1/2}.
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Q59MHT CET 2026 · 13 APR · SHIFT 2Medium

Velocity of Efflux (Torricelli)

The surface of water in a water tank of cross-section area 750750 cm2^{2} on the top of a house is hh m above the tap level. The speed of water coming out through the tap of cross-section area 500500 mm2^{2} is 3030 cm/s. At that instant, dh/dtdh/dt is y×10−3y \times 10^{-3} m/s. The value of yy will be

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Answer: (a)

  1. Continuity: A∣dhdt∣=avA\left|\frac{dh}{dt}\right| = a v
  2. ∣dhdt∣=(500×10−6)(0.30)750×10−4=1.5×10−40.075=2×10−3 m/s\left|\frac{dh}{dt}\right| = \frac{(500\times10^{-6})(0.30)}{750\times10^{-4}} = \frac{1.5\times10^{-4}}{0.075} = 2\times10^{-3}\text{ m/s}
  3. So the answer is (a) y=2y = 2.
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Q60JEE Main 2026 · 6 APR · SHIFT 2Medium

Velocity of Efflux (Torricelli)

A cylindrical vessel of 40 cm radius is completely filled with water and its capacity is 528 dm3528\text{ dm}^3 (dm: decimeter) The vessel is placed on a solid block of exactly same height as vessel. If a small hole is made at 70 cm below the top of water level, then horizontal range of water falling on the ground in the beginning is ______ cm.

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Answer: (b)

  1. Height of vessel: H=Vπr2=0.528227(0.4)2=1.05 m=105 cmH = \frac{V}{\pi r^2} = \frac{0.528}{\frac{22}{7}(0.4)^2} = 1.05\text{ m} = 105\text{ cm}
  2. Block has the same height, so the water top is 210 cm above the ground; the hole is at y=210−70=140y = 210 - 70 = 140 cm above ground, depth h=70h = 70 cm.
  3. Range: R=2h y=270×140=2×702=1402 cmR = 2\sqrt{h\,y} = 2\sqrt{70 \times 140} = 2 \times 70\sqrt{2} = 140\sqrt{2}\text{ cm}
  4. So the answer is (b) 1402140\sqrt{2}.
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Q61MHT CET 2026 · 20 APR · SHIFT 2Difficult

Velocity of Efflux (Torricelli)

On opposite sides of a wide vertical vessel filled with water (density ρ\rho), two identical holes are drilled, each having cross-section area AA. The height difference between holes is xx. The resultant force of reaction of water flowing out of vessel is (gg = acceleration due to gravity)

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Answer: (b)

jetjetF1F2x
  1. Reaction force of a jet: F=ρAv2=ρA(2gh)=2ρAghF = \rho A v^2 = \rho A(2gh) = 2\rho A g h
  2. The jets leave in opposite directions, so the reactions oppose each other.
  3. Net force: F2−F1=2ρAg(h2−h1)=2ρAgxF_2 - F_1 = 2\rho A g(h_2 - h_1) = 2\rho A g x
  4. So the answer is (b) 2ρAgx2\rho A g x.
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Q62MHT CET 2025 · 5 MAY · SHIFT 2Difficult

Velocity of Efflux (Torricelli)

A vessel completely filled with water has two holes ' P ' and ' Q ' at depths ' 2 h ' and ' 8 h ' from the top respectively. Hole ' P ' is square of side ' aa ' and hole ' QQ ' is a circle of radius ' rr '. The water flowing out per second from both the holes is same, then side ' aa ' of hole ' PP ' is

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Answer: (b)

  1. Volume flow rate Q=(area)×vQ = (\text{area}) \times v with efflux speed v=2gdv = \sqrt{2gd} at depth dd.
  2. Equal flow: a22g(2h)=πr22g(8h)a^2\sqrt{2g(2h)} = \pi r^2\sqrt{2g(8h)}
  3. a2=πr28h2h=2πr2a^2 = \pi r^2\sqrt{\frac{8h}{2h}} = 2\pi r^2
  4. So the answer is (b) a=r2πa = r\sqrt{2\pi}.
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Q63MHT CET 2025 · 22 APR · SHIFT 1Difficult

Velocity of Efflux (Torricelli)

There are two identical small holes on the opposite side of a tank containing full of a liquid. The tank is open at the top. The difference in height between the two holes is ' hh '. As the liquid comes out of the two holes, the tank will experience a net horizontal force proportional to

Figure

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Answer: (d)

  1. Each jet pushes the tank back with thrust F=ρav2F = \rho a v^2, and v2=2gdv^2 = 2gd at depth dd.
  2. The two jets point in opposite directions, so Fnet=ρa(v22−v12)=ρa⋅2g(d2−d1)F_{net} = \rho a(v_2^2 - v_1^2) = \rho a \cdot 2g(d_2 - d_1)
  3. d2−d1=h⇒Fnet=2ρaghd_2 - d_1 = h \Rightarrow F_{net} = 2\rho a g h
  4. So the answer is (d) Fnet∝hF_{net} \propto h.
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Q64NEET 2025Difficult

Velocity of Efflux (Torricelli)

Consider a water tank shown in the figure. It has one wall at x=Lx = L and can be taken to be very wide in the zz direction. When filled with a liquid of surface tension SS and density ρ\rho, the liquid surface makes angle θ0 (θ0≪1)\theta_0\ (\theta_0 \ll 1) with the xx-axis at x=Lx = L. If y(x)y(x) is the height of the surface then the equation for y(x)y(x) is:

Figure

(take θ(x)=sin⁡θ(x)=tan⁡θ(x)=dydx,g\theta(x) = \sin\theta(x) = \tan\theta(x) = \frac{dy}{dx}, g is the acceleration due to gravity)

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Answer: (d)

  1. For small slope, curvature of the surface is 1R=d2ydx2\frac{1}{R} = \frac{d^2y}{dx^2}, so the pressure jump across it is SR=Sd2ydx2\frac{S}{R} = S\frac{d^2y}{dx^2}.
  2. Liquid just below the surface at height yy (above the flat level) has pressure p0−ρgyp_0 - \rho g y.
  3. Balance: p0−(p0−ρgy)=Sd2ydx2p_0 - (p_0 - \rho g y) = S\frac{d^2y}{dx^2}
  4. So the answer is (d) d2ydx2=ρgSy\frac{d^2y}{dx^2} = \frac{\rho g}{S}y.
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Q65JEE Main 2025 · 3 APR · SHIFT 1Difficult

Velocity of Efflux (Torricelli)

Consider a completely full cylindrical water tank of height 1.6 m and of cross-sectional area 0.5 m20.5\text{ m}^2. It has a small hole in its side at a height 90 cm from the bottom. Assume, the cross-sectional area of the hole to be negligibly small as compared to that of the water tank. If a load 50 kg is applied at the top surface of the water in the tank then the velocity of the water coming out at the instant when the hole is opened is:

(g=10 m/s2)(g = 10\text{ m/s}^2)

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Answer: (d)

  1. Extra pressure from load: P=mgA=50×100.5=1000 PaP = \frac{mg}{A} = \frac{50 \times 10}{0.5} = 1000\text{ Pa}
  2. Depth of hole: h=1.6−0.9=0.7 mh = 1.6 - 0.9 = 0.7\text{ m}
  3. Bernoulli: 12ρv2=ρgh+P⇒v2=2(10×0.7+10001000)=16\frac{1}{2}\rho v^2 = \rho g h + P \Rightarrow v^2 = 2\left(10 \times 0.7 + \frac{1000}{1000}\right) = 16
  4. So the answer is (d) v=4 m/sv = 4\text{ m/s}.
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Q66MHT CET 2024 · 16 MAY · SHIFT 1Easy

Velocity of Efflux (Torricelli)

A cylinder contains water upto a height ' HH '. It has three orifices O1,O2,O3O_1, O_2, O_3 as shown in the figure. Let V1,V2,V3V_1, V_2, V_3 be the speed of efflux of water from the three orifices. Then

Figure

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Answer: (b)

  1. Torricelli: v=2ghv = \sqrt{2gh}, where hh is the depth of the orifice below the free surface.
  2. O1O_1 is shallowest and O3O_3 deepest, so h1<h2<h3h_1 < h_2 < h_3.
  3. So the answer is (b) V1<V2<V3V_1 < V_2 < V_3.
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Q67MHT CET 2024 · 10 MAY · SHIFT 1Medium

Velocity of Efflux (Torricelli)

A completely filled water tank of height ' hh ' has a hole at the bottom. The total pressure of the bottom is 4 H and atmospheric pressure is H. The velocity of water flowing out of the hole is ( ρ=\rho = density of water)

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Answer: (c)

  1. Gauge pressure at the bottom: ρgh=4H−H=3H\rho g h = 4H - H = 3H
  2. 12ρv2=3H⇒v=6Hρ\frac{1}{2}\rho v^2 = 3H \Rightarrow v = \sqrt{\frac{6H}{\rho}}
  3. So the answer is (c) 6Hρ\sqrt{\frac{6H}{\rho}}.
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Q68MHT CET 2024 · 4 MAY · SHIFT 1Medium

Velocity of Efflux (Torricelli)

The surface of water in a water tank of cross section area 750 cm2750\text{ cm}^2 on the top of a house is ' hh ' m\text{m} above the tap level. The speed of water coming out through the tap of cross section area 500 mm2500\text{ mm}^2 is 30 cm/s30\text{ cm/s}. At that instant dhdt\frac{dh}{dt} is x×10−3 m/sx \times 10^{-3}\text{ m/s}. The value of ' xx ' will be

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Answer: (a)

  1. Continuity: A∣dhdt∣=avA\left|\frac{dh}{dt}\right| = a v
  2. ∣dhdt∣=(500×10−6)(0.30)750×10−4=2×10−3 m/s\left|\frac{dh}{dt}\right| = \frac{(500\times10^{-6})(0.30)}{750\times10^{-4}} = 2\times10^{-3}\text{ m/s}
  3. So the answer is (a) x=2x = 2.
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Q69MHT CET 2024 · 3 MAY · SHIFT 1Medium

Velocity of Efflux (Torricelli)

A gardening pipe having an internal radius ' RR ' is connected to a water sprinkler having ' nn ' holes each of radius ' rr '. The water in the pipe has a speed ' vv '. The speed of water leaving the sprinkler is

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Answer: (b)

  1. Continuity: flow in the pipe = total flow out of nn holes
  2. πR2v=nπr2v′⇒v′=R2vnr2\pi R^2 v = n\pi r^2 v' \Rightarrow v' = \frac{R^2 v}{n r^2}
  3. So the answer is (b) R2vnr2\frac{R^2 v}{n r^2}.
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Q70JEE Main 2024 · 27 JAN · SHIFT 2Medium

Velocity of Efflux (Torricelli)

The reading of pressure metre attached with a closed pipe is 4.5×104 N/m24.5 \times 10^{4}\text{ N/m}^2. On opening the valve, water starts flowing and the reading of pressure metre falls to 2.0×104 N/m22.0 \times 10^{4}\text{ N/m}^2. The velocity of water is found to be V m/s\sqrt{V}\text{ m/s}. The value of VV is _________.

Numerical answer type. Work it out, then open the answer.

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Answer: 50

  1. Fall in static pressure becomes kinetic energy: ΔP=12ρv2\Delta P = \frac{1}{2}\rho v^2
  2. 4.5×104−2.0×104=12(1000)v2⇒v2=504.5\times10^{4} - 2.0\times10^{4} = \frac{1}{2}(1000)v^2 \Rightarrow v^2 = 50
  3. So V=50V = 50.
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Q71MHT CET 2023 · 13 MAY · SHIFT 2Medium

Velocity of Efflux (Torricelli)

There is hole of area AA at the bottom of a cylindrical vessel. Water is filled to a height hh and water flows out in tt second. If water is filled to a height 4h4h, it will flow out in time (in second)

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Answer: (c)

  1. Time to empty: t=AvesselA2hg⇒t∝ht = \frac{A_{vessel}}{A}\sqrt{\frac{2h}{g}} \Rightarrow t \propto \sqrt{h}
  2. t′t=4hh=2\frac{t'}{t} = \sqrt{\frac{4h}{h}} = 2
  3. So the answer is (c) 2t2t.
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Q72JEE Main 2023 · 1 FEB · SHIFT 2Medium

Velocity of Efflux (Torricelli)

The surface of water in a water tank of cross section area 750 cm2750\text{ cm}^2 on the top of a house is h mh\text{ m} above the tap level. The speed of water coming out through the tap of cross section area 500 mm2500\text{ mm}^2 is 30 cm/s30\text{ cm/s}. At that instant, dhdt\frac{dh}{dt} is x×10−3 m/sx \times 10^{-3}\text{ m/s}. The value of xx will be ____________.

Numerical answer type. Work it out, then open the answer.

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Answer: 2

  1. Continuity: A∣dhdt∣=avA\left|\frac{dh}{dt}\right| = a v
  2. ∣dhdt∣=(500×10−6)(0.30)750×10−4=2×10−3 m/s\left|\frac{dh}{dt}\right| = \frac{(500\times10^{-6})(0.30)}{750\times10^{-4}} = 2\times10^{-3}\text{ m/s}
  3. So x=2x = 2.
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Q73JEE Main 2022 · 28 JUL · SHIFT 2Medium

Velocity of Efflux (Torricelli)

Consider a cylindrical tank of radius 1 m1\text{ m} is filled with water. The top surface of water is at 15 m15\text{ m} from the bottom of the cylinder. There is a hole on the wall of cylinder at a height of 5 m5\text{ m} from the bottom. A force of 5×105 N5 \times 10^{5}\text{ N} is applied on the top surface of water using a piston. The speed of efflux from the hole will be: (given atmospheric pressure PA=1.01×105 PaP_A = 1.01 \times 10^{5}\text{ Pa}, density of water ρW=1000 kg/m3\rho_W = 1000\text{ kg/m}^3 and gravitational acceleration g=10 m/s2g = 10\text{ m/s}^2)

Figure

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Answer: (c)

  1. Extra pressure from the piston: Fπr2=5×105π(1)2≈1.59×105 Pa\frac{F}{\pi r^2} = \frac{5\times10^{5}}{\pi(1)^2} \approx 1.59\times10^{5}\text{ Pa}
  2. Full Bernoulli (top to hole, depth 10 m): 12ρv2=FA+ρg(10)=1.59×105+1.0×105⇒v≈22.8 m/s\frac{1}{2}\rho v^2 = \frac{F}{A} + \rho g(10) = 1.59\times10^{5} + 1.0\times10^{5} \Rightarrow v \approx 22.8\text{ m/s} (not among the options)
  3. The official answer uses only the piston pressure: 12ρv2=1.59×105⇒v=318≈17.8 m/s\frac{1}{2}\rho v^2 = 1.59\times10^{5} \Rightarrow v = \sqrt{318} \approx 17.8\text{ m/s}
  4. So the answer is (c) 17.8 m/s.
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Q74JEE Main 2022 · 27 JUN · SHIFT 1Medium

Velocity of Efflux (Torricelli)

The area of cross-section of a large tank is 0.5 m2. It has a narrow opening near the bottom having area of cross-section 1 cm2. A load of 25 kg is applied on the water at the top in the tank. Neglecting the speed of water in the tank, the velocity of the water, coming out of the opening at the time when the height of water level in the tank is 40 cm above the bottom, will be ___________ cms−1{}^{-1}. [Take g = 10 ms−2{}^{-2}]

Numerical answer type. Work it out, then open the answer.

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Answer: 300

  1. Extra pressure from the load: mgA=25×100.5=500 Pa\frac{mg}{A} = \frac{25 \times 10}{0.5} = 500\text{ Pa}
  2. Bernoulli: 12ρv2=mgA+ρgh=500+1000(10)(0.4)=4500\frac{1}{2}\rho v^2 = \frac{mg}{A} + \rho g h = 500 + 1000(10)(0.4) = 4500
  3. v2=9⇒v=3 m/s=300 cm/sv^2 = 9 \Rightarrow v = 3\text{ m/s} = 300\text{ cm/s}
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Q75JEE Main 2021 · 27 JUL · SHIFT 2Medium

Velocity of Efflux (Torricelli)

The water is filled upto height of 12 m in a tank having vertical sidewalls. A hole is made in one of the walls at a depth 'h' below the water level. The value of 'h' for which the emerging steam of water strikes the ground at the maximum range is ________ m.

Numerical answer type. Work it out, then open the answer.

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Answer: 6

  1. Hole at depth hh, height above ground H−hH - h: range R=2h(H−h)R = 2\sqrt{h(H - h)}
  2. RR is maximum when h=H−h⇒h=H2h = H - h \Rightarrow h = \frac{H}{2}
  3. h=122=6 mh = \frac{12}{2} = 6\text{ m}
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Q76JEE Main 2021 · 18 MAR · SHIFT 2Medium

Velocity of Efflux (Torricelli)

Consider a water tank as shown in the figure. It's cross-sectional area is 0.4 m2. The tank has an opening B near the bottom whose cross-section area is 1 cm2. A load of 24 kg is applied on the water at the top when the height of the water level is 40 cm above the bottom, the velocity of water coming out the opening B is v ms-1.

The value of v, to the nearest integer, is ___________. [Take value of g to be 10 ms-2]

Figure

Numerical answer type. Work it out, then open the answer.

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Answer: 3

  1. Extra pressure from the load: mgA=24×100.4=600 Pa\frac{mg}{A} = \frac{24 \times 10}{0.4} = 600\text{ Pa}
  2. Bernoulli: 12ρv2=600+1000(10)(0.4)=4600\frac{1}{2}\rho v^2 = 600 + 1000(10)(0.4) = 4600
  3. v2=9.2⇒v≈3.03 m/sv^2 = 9.2 \Rightarrow v \approx 3.03\text{ m/s}
  4. So v≈3v \approx 3.
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Q77JEE Main 2021 · 27 JUL · SHIFT 1Difficult

Velocity of Efflux (Torricelli)

A light cylindrical vessel is kept on a horizontal surface. Area of base is A. A hole of cross-sectional area 'a' is made just at its bottom side. The minimum coefficient of friction necessary to prevent sliding the vessel due to the impact force of the emerging liquid is (a < < A):

Figure

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Answer: (c)

  1. Efflux speed v=2ghv = \sqrt{2gh}, so the jet's reaction force is F=ρav2=2ρaghF = \rho a v^2 = 2\rho a g h.
  2. Vessel is light, so normal force = weight of liquid: N=ρAhgN = \rho A h g.
  3. No sliding: μN≥F⇒μ≥2ρaghρAhg=2aA\mu N \ge F \Rightarrow \mu \ge \frac{2\rho a g h}{\rho A h g} = \frac{2a}{A}
  4. So the answer is (c) 2aA\frac{2a}{A}.
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Q78MHT CET 2020 · 16 OCT · SHIFT 2Medium

Velocity of Efflux (Torricelli)

A large open tank containing water has two holes to its wall. A square hole of side aa is made at a depth yy and a circular hole of radius rr is made at a depth 16y16y from the surface of water. If equal amount of water comes out through both the holes per second, then the relation between rr and aa will be

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Answer: (a)

  1. Equal flow: a22gy=πr22g(16y)a^2\sqrt{2gy} = \pi r^2\sqrt{2g(16y)}
  2. a2=4πr2⇒r=a2πa^2 = 4\pi r^2 \Rightarrow r = \frac{a}{2\sqrt{\pi}}
  3. So the answer is (a) r=a2πr = \frac{a}{2\sqrt{\pi}}.
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Q79NEET 2019Easy

Velocity of Efflux (Torricelli)

A small hole of area of cross-section 2 mm2 present near the bottom of a fully filled open tank of height 2 m. Taking g = 10 m/s2, the rate of flow of water through the open hole would be nearly:

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Answer: (d)

  1. Torricelli: v=2gh=2(10)(2)=40≈6.32 m/sv = \sqrt{2gh} = \sqrt{2(10)(2)} = \sqrt{40} \approx 6.32\text{ m/s}
  2. Q=av=(2×10−6)(6.32)≈12.6×10−6 m3/sQ = av = (2\times10^{-6})(6.32) \approx 12.6\times10^{-6}\text{ m}^3\text{/s}
  3. So the answer is (d) 12.6×10−612.6\times10^{-6} m3^3/s.
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Q80JEE Main 2019 · 10 JAN · SHIFT 1Medium

Velocity of Efflux (Torricelli)

Water flows into a large tank with flat bottom at the rate of 10–4m3s–1. Water is also leaking out of a hole ofarea 1 cm2 at its bottom. If the height of the water in the tank remains steady, then this height is -

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Answer: (b)

  1. Steady level: inflow = outflow, Q=a2ghQ = a\sqrt{2gh}
  2. 2gh=10−410−4=1 m/s\sqrt{2gh} = \frac{10^{-4}}{10^{-4}} = 1\text{ m/s}
  3. h=12(9.8)≈0.051 m=5.1 cmh = \frac{1}{2(9.8)} \approx 0.051\text{ m} = 5.1\text{ cm}
  4. So the answer is (b) 5.1 cm.
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Q81JEE Main 2019 · 9 JAN · SHIFT 2Medium

Velocity of Efflux (Torricelli)

The top of a water tank is open to air and its water level is mainted. It is giving out 0.74 m3 water per minute through a circular opening of 2 cm radius in its wall. The depth of the center of the opening from the level of water in the tank is close to:

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Answer: (b)

  1. Q=0.7460=1.23×10−2 m3/sQ = \frac{0.74}{60} = 1.23\times10^{-2}\text{ m}^3\text{/s}, a=π(0.02)2=1.26×10−3 m2a = \pi(0.02)^2 = 1.26\times10^{-3}\text{ m}^2
  2. v=Qa≈9.8 m/sv = \frac{Q}{a} \approx 9.8\text{ m/s}
  3. h=v22g=962(10)≈4.8 mh = \frac{v^2}{2g} = \frac{96}{2(10)} \approx 4.8\text{ m}
  4. So the answer is (b) 4.8 m.
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Q82JEE Main 2016 · 9 APR · SHIFT 1Difficult

Velocity of Efflux (Torricelli)

Figure

Consider a water jar of radius R that has water filled up to height H and is kept on astand of height h (see figure). Through a hole of radius r (r << R) at its bottom, the water leaks out and the stream of water coming down towards the ground has a shape like a funnel as shown in the figure. If the radius of the cross-section of water stream when it hits the ground is x. Then:

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Answer: (c)

  1. Speed at the hole: v1=2gHv_1 = \sqrt{2gH}; speed at the ground: v2=2g(H+h)v_2 = \sqrt{2g(H+h)}.
  2. Continuity: πr2v1=πx2v2⇒x2=r2HH+h\pi r^2 v_1 = \pi x^2 v_2 \Rightarrow x^2 = r^2\sqrt{\frac{H}{H+h}}
  3. So the answer is (c) x=r(HH+h)1/4x = r\left(\frac{H}{H+h}\right)^{1/4}.
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Q83NEET 2015 · AIPMTMedium

Velocity of Efflux (Torricelli)

The cylindrical tube of a spray pump has radius R, one end of which has n fine holes, each of radius r. If the speed of the liquid in the tube is V, the speed of the ejection of the liquid through the holes is

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Answer: (d)

  1. Continuity: πR2V=nπr2v\pi R^2 V = n\pi r^2 v
  2. v=VR2nr2v = \frac{VR^2}{nr^2}
  3. So the answer is (d) VR2nr2\frac{VR^2}{nr^2}.
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Q84JEE Main 2014 · 12 APR · SHIFT 1Medium

Velocity of Efflux (Torricelli)

A cylindrical vessel of cross-section A contains water to a height h. There is a hole in the bottom of radius 'a'. The time in which it will be emptied is:

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Answer: (b)

  1. Continuity: −Adhdt=πa22gh-A\frac{dh}{dt} = \pi a^2\sqrt{2gh}
  2. Integrate from hh to 0: t=Aπa2⋅2h2g=Aπa22hgt = \frac{A}{\pi a^2}\cdot\frac{2\sqrt{h}}{\sqrt{2g}} = \frac{A}{\pi a^2}\sqrt{\frac{2h}{g}}
  3. t=2Aπa2hgt = \frac{\sqrt{2}A}{\pi a^2}\sqrt{\frac{h}{g}}
  4. So the answer is (b).
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Q85JEE Main 2014 · 11 APR · SHIFT 1Medium

Velocity of Efflux (Torricelli)

A tank with a small hole at the bottom has been filled with water and kerosene (specific gravity 0.8). The height of water is 3 m and that of kerosene 2 m. When the hole is opened the velocity of fluid coming out from it is nearly: (take g = 10 ms−2{}^{-2} and density of water = 103 kg m−3{}^{-3})

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Answer: (b)

  1. Gauge pressure at the bottom: ρkghk+ρwghw=800(10)(2)+1000(10)(3)=46000 Pa\rho_k g h_k + \rho_w g h_w = 800(10)(2) + 1000(10)(3) = 46000\text{ Pa}
  2. Bernoulli at the hole: 12ρwv2=46000⇒v2=92\frac{1}{2}\rho_w v^2 = 46000 \Rightarrow v^2 = 92
  3. v≈9.6 m/sv \approx 9.6\text{ m/s}
  4. So the answer is (b) 9.6 m s−1^{-1}.
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Q86JEE Main 2002 · AIEEEEasy

Velocity of Efflux (Torricelli)

A cylinder of height 20 m20\text{ m} is completely filled with water. The velocity of efflux of water (in ms−1\text{ms}^{-1}) through a small hole on the side wall of the cylinder near its bottom is

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Answer: (b)

  1. Torricelli: v=2gh=2(9.8)(20)=392≈19.8≈20 m/sv = \sqrt{2gh} = \sqrt{2(9.8)(20)} = \sqrt{392} \approx 19.8 \approx 20\text{ m/s}
  2. So the answer is (b) 20.
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